Novel Hydroxyapatite Beads for the Adsorption of Radionuclides from Decommissioned Nuclear Power Plant Sites

: Although a powdered form of hydroxyapatite (p-HdA) has been studied for the adsorption of heavy metals that contaminate the restoration sites of decommissioned nuclear power plants, most of the studies are limited in the laboratory due to the head loss and post-separation in practical applications. Herein, we fabricated a porous bead form of HdA (b-HdA) as a novel adsorbent for removing radionuclides from aqueous environments via a facile synthesis by mixing the p-HdA precursor and polyvinyl butyral (PVB) as a binder and added a sintering process for the ﬁnal production of a porous structure. The spherical b-HdA with an approximate diameter of 2.0 mm was successfully fabricated. The effectiveness of the b-HdA at removing Co(II) was investigated via the adsorption equilibrium at various experimental temperatures. The b-HdA exhibited the adsorption capacity for Co(II) ions with a maximum of 7.73 and 11.35 mg/g at 293 K and 313 K, respectively. The experimental kinetic data were well described using a pseudo-second-order kinetic model, and the adsorption mechanisms of Co(II) onto the b-HdA were revealed to be a chemisorption process with intraparticle diffusion being the rate-limiting step. In addition, the competitive adsorption onto the b-HdA with the order of U(VI) > Co(II) > Ni(II) > Sr(II) > Cs(I) was also observed in the multi-radionuclides system. Considering the advantages of the size, applicability to the continuous-ﬂow column, and the easy separation from treated water, the b-HdA can be an excellent absorbent with high potential for practical applications for removing radionuclides.


Introduction
In recent years, increasing attention has been paid to the removal of radioactive pollutants from aquatic ecosystems due to their frequent and widespread detection [1,2]. In addition to natural radionuclides, the occurrence of radioactive pollutants has become widely recognized due to their introduction through anthropogenic sources, such as nuclear power plants, weapons, medicine, industrial radiography, studies, accidental releases, and inadequate practices of radioactive waste disposal [3][4][5]. Among the various noxious radionuclides, 137 Cs, 60 Co, 63 Ni, 55 Fe, 90 Sr, 226 Ra, 232 Th, and 238 U were reported as the key artificial radioactive contaminants [1][2][3]. Remarkably, 60 Co has been identified as a significant environmental issue because it generally prevailed in aqueous wastes that are discharged from nuclear facilities [3,6]. Ionizing radiation exposure has emerged as a serious public health issue due to its biologically dynamic toxicity via generating free radicals, which can damage, mutate, or even kill cells [7,8]. Although cobalt is a micronutrient, excessive cobalt exposure results in various health hazards, such as neurological and cardiovascular issues, endocrine deficits, bone defects, and cancers [4]. Given the harmful nature of such radionuclides, various methods have been proposed and developed to effectively control radionuclide ions in contaminated water, including reverse osmosis, membrane separation, adsorption, biological treatment, and electrodialysis [3,5,7,8]. Among them, adsorption has been widely investigated as the most cost-effective, environmentally friendly method and the easiest technique for industrial application [9,10]. In this regard, various types of adsorbents, including biomass, clays, activated carbon, hydroxyapatite, metal particulates, and metal oxides functionalized with bio-based substances have been used to separate contaminants during water treatment [1,5,11].
Of them, hydroxyapatite (Ca 10 (PO 4 ) 6 (OH) 2 ), a calcium phosphate, has emerged as one of the promising environmental remediation materials with low cost, nontoxicity, biocompatibility, and biodegradability properties [12]. The popularity lies in its particular structure and unique properties, such as its ion exchange capability, adsorptive ability, acidbase adjustability, and thermal stability [12][13][14][15][16]. The feasibility of hydroxyapatite (HdA) nanoparticles as effective adsorbents is well documented for the adsorption of various multi-valent metal ions, such as lead, cobalt, nickel, copper, zinc, cadmium, strontium, and uranium [1,[17][18][19]. Indeed, the HdA has a versatile structure, which allows foreign ions to substitute Ca-ions on the framework without any distortion [20]. Nevertheless, the use of HdA nanoparticles in the industrial field is limited due to their difficulties in separating them from effluent and the possibility of causing secondary pollution [12]. The auxiliary separation steps, such as ultrafiltration or the sedimentation process, requires a significant amount of time, additional investment, and operation costs [21]. In addition, the application of powdered hydroxyapatite (p-HdA) for the continuous-flow column is impossible due to the significant head loss that is induced by the small size of HdA powders. Taking into account these issues, the fabrication of macro-sized HdA granules will enable easier separation in suspended applications, as well as lower head-loss during continuous-flow column applications.
For biomedical applications, several methods have been employed to fabricate a macro-structured HdA, such as granulating via centrifugation and vibration, sintering, casting in plaster molds, and spraying [22][23][24]. Regarding environmental applications, only a few studies have been developed for water treatment so far. Nijhawan et al. [25,26] fabricated porous HdA ceramic beads (4.0-5.0 mm) by mixing the p-HdA and solute starch and sintering at 1200 • C for 2 h to adsorb the fluoride. Le et al. [27] mixed the p-HdA and polyvinyl alcohol (PVA) and calcinated at 600 • C for 4 h to obtain HdA pellets (2.0 × 10.0 mm) with a maximum lead adsorption capacity of 7.99 mg/g.
In this work, a facile and rapid preparation method for fabricating macro-sized HdA beads was developed from a mixture of polyvinyl butyral (PVB) and HdA for the application of continuous flow columns, and the adsorption of radionuclides, such as Co(II), ions in a single and multi-ionic system to simulate the treatability of radionuclides that originate from the decommissioning sites of nuclear power plants was verified. The equilibrium, kinetic, and thermodynamic adsorption experiments of b-HdA were conducted for Co(II) ions, and the experimental data were fitted with various equilibrium isotherms and kinetic models to obtain a deeper understanding of the adsorption behaviors and mechanisms.

Preparation of Porous HdA Beads
The porous bead form of HdA (b-HdA) was fabricated by using the sintering method with p-HdA as a precursor and PVB as a binder and pore-forming agent. A mixture containing 2.0 g of PVB and 18.0 g NMP was first prepared via magnetic stirring for 24 h at room temperature. Then, 15.0 g of p-HdA and 16.0 g of NMP were added into the mixture, subsequently sonicated for 60 min, and continuously mixed for 24 h. After homogenization, the mixture was poured into a 50 mL disposable KOVAX syringe (Henke Sass Wolf GmbH, Tuttlingen, Germany) and extruded using a KDS230 syringe pump (KD Scientific Inc., Holliston, MA, USA) with a flow rate of 1 mL/min. The spherical b-HdA was formed when the mixture was added dropwise into deionized water (DIW) and cured for 1 h. After the hardening stage, we rinsed the b-HdA three times with DIW and then dried it overnight at room temperature. Finally, the produced b-HdA was calcinated at 550 • C for 2 h to remove the PVB and residual organic compounds.

Adsorption Experiments
The adsorption equilibrium was carried out with 300 mL glass bottles containing The adsorption capacity of radionuclides (q e (mg/g)) was calculated using the following mass balance equation [28]: where C o and C e (mg/L) are the initial and equilibrium concentrations of the adsorbate, respectively, V (L) is the volume of the adsorbate solution, and m (g) is the mass of the b-HdA used.

Material Characterization
The surface morphology of the prepared b-HdA was acquired using a field emission scanning electron microscope (FESEM, SU8230, Hitachi Corp., Tokyo, Japan) equipped with an energy-dispersive X-ray spectroscope (EDX). The Brunauer-Emmett-Teller (BET) specific area, the Barrett-Joyner-Halenda (BJH) pore size, and the pore volume were measured using a BELSORP MAX surface analyzer (MicrotracBEL Corp., Tokyo, Japan). The X-ray diffraction (XRD) of the adsorbents were examined using a RIGAKU diffractometer (D/MAX-2500, Tokyo, Japan) scanned over the range of 2θ = 5 − 80 • with a Cu Kα radiation source (λ = 1.5418 Å). The pH of the point of zero charge (pHpzc) of the b-HdA was checked using the pH drift method [29]. Briefly, 0.15 g of the b-HdA were embedded in a 40 mL solution with pH's ranging from 2 to 11. After 24 h of shaking at 150 rpm, the pH stabilized and we measured the final pH. The pHpzc was determined as the point at which the initial pH and final pH values were equal.

Adsorption Data Analysis
In this presented work, the experimental equilibrium data were analyzed using four well-known isothermal models, namely, the Langmuir, Freundlich, Sips, and Tempkin isotherm models [9,30]. The mathematical expressions of these models are given in Table S1. To determine the possible nature of the adsorption process, the thermodynamic parameters were defined using equations in Table S2. A more detailed explanation can be found in our previous publication [31]. The experimental kinetic data were evaluated using the pseudo-first-order, pseudo-second-order, intra-particle diffusion, and three-stage models to determine the type of mechanism and potential rate-controlling step of the adsorption processes [9,32,33]. These kinetic equations are presented in Table S3.

Physico-Chemical Properties of the Prepared b-HdA
The nitrogen adsorption-desorption isotherms of the p-HdA and b-HdA are presented in Figure 1a. Both the p-HdA and b-HdA exhibited type IV isotherms with type H 3 hysteresis loops, suggesting that the materials had mesoporous structures with the aggregates of particles forming slit-like pores [34,35]. The BJH pore size distribution curves illustrated in Figure 1b confirmed that mesopores were predominant for both materials. It can also be seen from Figure 1b that the p-HdA had a broader pore size distribution compared to the HdA pellets.
in a 40 mL solution with pH's ranging from 2 to 11. After 24 h of shaking at 150 rpm, the pH stabilized and we measured the final pH. The pHpzc was determined as the point a which the initial pH and final pH values were equal.

Adsorption Data Analysis
In this presented work, the experimental equilibrium data were analyzed using four well-known isothermal models, namely, the Langmuir, Freundlich, Sips, and Tempkin isotherm models [9,30]. The mathematical expressions of these models are given in Table  S1. To determine the possible nature of the adsorption process, the thermodynamic pa rameters were defined using equations in Table S2. A more detailed explanation can be found in our previous publication [31]. The experimental kinetic data were evaluated us ing the pseudo-first-order, pseudo-second-order, intra-particle diffusion, and three-stage models to determine the type of mechanism and potential rate-controlling step of the ad sorption processes [9,32,33]. These kinetic equations are presented in Table S3.

Physico-Chemical Properties of the Prepared b-HdA
The nitrogen adsorption-desorption isotherms of the p-HdA and b-HdA are pre sented in Figure 1a. Both the p-HdA and b-HdA exhibited type IV isotherms with type H hysteresis loops, suggesting that the materials had mesoporous structures with the aggre gates of particles forming slit-like pores [34,35]. The BJH pore size distribution curves il lustrated in Figure 1b confirmed that mesopores were predominant for both materials. I can also be seen from Figure 1b that the p-HdA had a broader pore size distribution com pared to the HdA pellets. The mean pore diameters of p-HdA and b-HdA were 16.22 nm and 22.73 nm, respectively, as presented in Table 1. The BET specific surface area of the b-HdA was half that of the p-HdA, which could be foreseen due to the effect of particle size on the BET specific  The mean pore diameters of p-HdA and b-HdA were 16.22 nm and 22.73 nm, respectively, as presented in Table 1. The BET specific surface area of the b-HdA was half that of the p-HdA, which could be foreseen due to the effect of particle size on the BET specific surface area [36]. The XRD patterns of the p-HdA and b-HdA presented in Figure 1c matched well with the standard patterns of the hexagonal crystal hydroxyapatite compiled by the International Centre for Diffraction Data (ICDD) card no. 01-074-0565 and 01-082-2956, respectively. The sharp, narrow, and well-resolved diffraction peaks observed in Figure 1c corresponded to the Miler indices of 100, 002, 210, 211, 112, 300, 202, 130, 222, 132, 213, 321, and 004, respectively, confirming the crystallized structure of the materials [37,38]. Furthermore, no additional peaks were found in the diffraction pattern of the b-HdA, indicating that hydroxyapatite was the only phase and PVB completely decomposed into volatile products at 550 • C [39]. Furthermore, a slightly higher intensity of the diffraction peaks was obtained for b-HdA compared to that of p-HdA, which might have resulted from the fact that the sintering process improved the crystallinity of the material [40]. Figure 1d shows that the pH pzc of the b-HdA was 7.9, which was similar to the precursor-HdA powder and other previous studies [38,41,42]. However, it is noteworthy to mention that the pH pzc of the HdA can fall in a wide range (4.3-9.2) depending on the synthesized method, HdA precursor, stoichiometry and purity, experimental conditions, and techniques [21,43]. It has also been reported that the pH pzc value of the HdA correlates proportionally with the quantity of Ca in the HdA surface [44].

Adsorption Isotherms
The adsorption parameters that were attained by fitting the equilibrium adsorption data with the four selected isotherm models are summarized in Table 2. The regression coefficient (R 2 ) values of the four adsorption isotherms in Table 2 show that the Sips, Freundlich, and Langmuir models provided better fits than the Tempkin model. Among  HdA (a,c) and b-HdA (b,d).

Adsorption Isotherms
The adsorption parameters that were attained by fitting the equilibrium adsorption data with the four selected isotherm models are summarized in Table 2. The regression coefficient (R 2 ) values of the four adsorption isotherms in Table 2 show that the Sips, Freundlich, and Langmuir models provided better fits than the Tempkin model. Among these models, the Sips model was adapted to explain the uptake behavior of Co(II) onto the b-HdA.  Figure 3 presents the equilibrium adsorption data fitted using the Sips adsorption model at different experimental temperatures. The maximum adsorption capacity (q max ) of the b-HdA that was calculated from the Sips isotherm for Co(II) ions at 293 K was 7.73 mg/g, which was about half that for p-HdA (14.07 mg/g) due to b-HdA's smaller BET specific surface area. The Sips model was developed from the basis of the Freundlich and Langmuir models, which are described by the dimensionless heterogeneity factor n s . At values of n s close to (or exactly) 1, the Sips isotherm approaches the Langmuir isotherm, which suggests homogeneous adsorption. From Table 2, it was found that the value of n s was much lower than 1 for all investigated temperatures, indicating that the b-HdA had an energetically heterogeneous surface [9]. It is believed that this heterogeneity was caused by the distinct binding sites present on the HdA surface, i.e., positively charged calcium ions and negatively charged hydroxyl, together with phosphate groups [1,20,44]. Consequently, different possible adsorption mechanisms can take place during the adsorption process, i.e., ion exchange and dissolution-precipitation according to Equations (2)-(4) [6,20]. Ca 10 (PO 4 ) 6 (OH) 2 + 2Co 2+ → Ca 8 Co 2 (PO 4 ) 6 (OH) 2 + 2Ca 2+ , Ca 10 (PO 4 ) 6 (OH) 2 10Co 2+ + 6H 2 PO 4 − + 2H 2 O → Co 10 (PO 4 ) 6 (OH) 2 + 14H + .
The comparison of adsorption capacities of Co(II) using various adsorbents is presented in Table 3. It can be seen that the adsorption capacity of Co(II) by the b-HdA fabricated in this study was lower than that of other HdA-based adsorbents due to its larger size. Nevertheless, the b-HdA exhibited higher adsorption capacity than other granular adsorbents, such as activated carbon [45] and clinoptilolite [46]. This finding suggested that the b-HdA can serve as a competent adsorbent for practical applications in the removal of Co(II) from contaminated water. The comparison of adsorption capacities of Co(II) using various adsorbents is presented in Table 3. It can be seen that the adsorption capacity of Co(II) by the b-HdA fabricated in this study was lower than that of other HdA-based adsorbents due to its larger size. Nevertheless, the b-HdA exhibited higher adsorption capacity than other granular adsorbents, such as activated carbon [45] and clinoptilolite [46]. This finding suggested that the b-HdA can serve as a competent adsorbent for practical applications in the removal of Co(II) from contaminated water. In addition, an increase in the adsorption capacity was observed with an increase in the experimental temperature from 293 to 313 K. This implies that the adsorption process was endothermal in nature and for the analysis that follows.

Thermodynamic Study
Thermodynamic studies were performed to determine the nature of the adsorption processes. In this work, the thermodynamic equilibrium constants (K 0 ) were calculated via ln(K 0 ) at different investigated temperatures (293, 303, and 313 K) by plotting ln(C s /C e ) versus C s and extrapolating C s to zero, as illustrated in Figure 4a [30]. The standard enthalpy change (∆H 0 ) and the standard entropy change (∆S 0 ) of the adsorption process were respectively obtained from the slope (−∆H 0 /R) and the intercept (∆S 0 /R) of the plots of ln(K 0 ) as a function of 1/T, as shown in Figure 4b.
Thermodynamic studies were performed to determine the nature of the adsorption processes. In this work, the thermodynamic equilibrium constants (K0) were calculated via ln(K0) at different investigated temperatures (293, 303, and 313 K) by plotting ln(Cs/Ce) versus Cs and extrapolating Cs to zero, as illustrated in Figure 4a [30]. The standard enthalpy change (ΔH 0 ) and the standard entropy change (ΔS 0 ) of the adsorption process were respectively obtained from the slope (−ΔH 0 /R) and the intercept (ΔS 0 /R) of the plots of ln(K0) as a function of 1/T, as shown in Figure 4b.  The calculated parameters are summarized in Table 4. The positive value of enthalpy ΔH 0 confirmed the endothermic nature of the adsorption process. As a result, the adsorption of Co(II) onto the b-HdA was favorable at high temperatures [31]. Furthermore, the positive value of entropy ΔS 0 indicates that the randomness at the b-HdA and solution interface increased during the adsorption process due to the release of the solvated water molecules present on the surface of the b-HdA [38]. Furthermore, the negative values of the standard Gibbs free energy change (ΔG 0 ) at all investigated temperatures indicated  Table 4. The positive value of enthalpy ∆H 0 confirmed the endothermic nature of the adsorption process. As a result, the adsorption of Co(II) onto the b-HdA was favorable at high temperatures [31]. Furthermore, the positive value of entropy ∆S 0 indicates that the randomness at the b-HdA and solution interface increased during the adsorption process due to the release of the solvated water molecules present on the surface of the b-HdA [38]. Furthermore, the negative values of the standard Gibbs free energy change (∆G 0 ) at all investigated temperatures indicated that the adsorption of Co(II) ions onto the b-HdA was thermodynamically favorable and spontaneous [38].

Adsorption Kinetics
Figure 5a elucidates the fitting of the pseudo-second-order and three-stage kinetic models with the experimental kinetics data for the adsorption of Co(II) onto the b-HdA. The correlation coefficients (R 2 ) in Table 5 show a better fit to the pseudo-second-order than the pseudo-first-order model, revealing that the pseudo-second-order model was more suitable for describing the kinetic mechanisms of Co(II) adsorption onto the b-HdA. Hence, the Co(II) adsorbed onto the adsorbent might have been controlled by a chemisorption step. Furthermore, the adsorption behavior of Co(II) on the exterior and interior adsorptive sites of the HdA pellets was revealed through the three-stage kinetic model. The threestage model considers three different adsorption stages, including the first (sharp) portion reflecting external mass transfer, the second (gradual) portion representing the internal surface adsorption (intraparticle diffusion), and the third (constant) portion denoting the equilibrium stage [9,32]. It can be seen from Figure 5a that the C t /C o values achieved from the calculations of the three-stage model were very close to the experimental data. In addition, a significantly lower instantaneous adsorption portion (ξ 1 ) compared to the interior adsorption portion (ξ 2 ) indicates that a major part of the adsorption occurred on the internal adsorptive sites of the b-HdA, as presented in Table 5 [32]. Consequently, the mechanism controlling the process might have been intraparticle diffusion [32,43].
Furthermore, the value of ξ 1 was very small, suggesting that the external surface adsorption of Co(II) ions occurred rapidly and that the adsorption process quickly progressed to the intraparticle diffusion stage [9].
tion denoting the equilibrium stage [9,32]. It can be seen from Figure 5a that the Ct/Co values achieved from the calculations of the three-stage model were very close to the experimental data. In addition, a significantly lower instantaneous adsorption portion (ξ1) compared to the interior adsorption portion (ξ2) indicates that a major part of the adsorption occurred on the internal adsorptive sites of the b-HdA, as presented in Table 5 [32]. Consequently, the mechanism controlling the process might have been intraparticle diffusion [32,43]. Furthermore, the value of ξ1 was very small, suggesting that the external surface adsorption of Co(II) ions occurred rapidly and that the adsorption process quickly progressed to the intraparticle diffusion stage [9].    Figure 5b shows the graph of q t versus t 0.5 , which fits the experimental data with the intraparticle diffusion model. The plot presents a linearized section (i.e., red dotted line) during the second (gradual) portion of the adsorption process, which indicates that intraparticle diffusion took place in the rate-limiting step. This result is consistent with the data obtained from the three-stage kinetic model (discussed above). However, the plot did not pass through the origin (I = 0); thus, intraparticle diffusion was not the sole rate-controlling step of the adsorption process [30]. It is noteworthy that two linearity fractions with different slopes corresponding to different stages in the adsorption process were observed in Figure 5b, implying that the multi-kinetic stage might have governed the adsorption of Co(II) onto the b-HdA.

Comparability and Selectivity of the b-HdA in a Multi-Ionic System
Several radionuclide ions, such as Ni(II), Sr(II), Cs(I), and U(VI), have frequently been detected in groundwater and wastewater, which might significantly affect the adsorption behavior of Co(II) [3]. We observed that the removal efficiencies of Co(II) decreased consid-erably in the multi-ionic systems compared to those in the single systems (data not shown), which could be attributed to competing effects. Furthermore, the selective order in the adsorption of these radionuclides on the b-HdA was U(VI) > Co(II) > Ni(II) > Sr(II) > Cs(I), as illustrated in Figure 6a,b. Research has shown that the absorption preference is affected by various characteristics of the adsorbates, such as ionic valence, ionic radius, hydration radius, electronegativity, hydration enthalpy, and charge density [6,40,44]. Generally, the adsorptive sites are preferentially occupied by ions with higher electronegativity, bigger ionic radius and valence, and smaller hydration radius [12]. Furthermore, ions with a higher hydration enthalpy prefer the solution phase, where it may satisfy its hydration requirements. In contrast, ions with a lower hydration enthalpy prefer the adsorbent phase [12]. In this respect, the characteristic parameters of the investigated radionuclides ions are presented in Table S4. It can be observed that even the trends could not provide a consistent rule for examined radionuclides' selectivities for the b-HdA. Nevertheless, it is noteworthy that the selective order of examined ions only coincided with the order trend of charge density, which was U(VI) > Co(II) > Ni(II) > Sr(II) > Cs(I), suggesting that the adsorption affinity might more strongly depend on the charge density of ions than other characteristics. It was reported that ions with a larger charge density are capable of substituting Ca(II) ions on the HdA surface more easily and quickly than others [3,19,47]. Considering that ion exchange takes place as the main adsorption mechanism, this postulation is a reasonable way to interpret the selectivity of the adsorption process in this work. Our results are consistent with previous studies using hydroxyapatite-based materials as adsorbents for the uptake of metal ions [3,17,48].

Conclusions
In this work, spherical b-HdA with an approximate diameter of 2.0 mm was successfully prepared via a sintering process. The prepared b-HdA had a well-crystallized and mesoporous structure with a BET specific surface area of 34.91 m 2 /g and a maximum specific adsorption of 7.73 mg/g b-HdA for Co(II) at 293 K. The adsorption behaviors and mechanisms of Co(II) ions onto the b-HdA could be explained well using the Sips isotherm model and the pseudo-second-kinetic model, indicating the heterogeneous surface property of b-HdA. The adsorption capacity was increased with an increase in temperature, along with the thermodynamic parameters, indicating that the adsorption of Co(II) onto the b-HdA was thermodynamically favorable and spontaneous. Furthermore, intraparticle diffusion controlled the uptake of Co(II) onto the b-HdA as a rate-limiting step. The selective order of the b-HdA in a mixture of radionuclides was U(VI) > Co(II) > Ni(II) > Sr(II) > Cs(I) due to the impact of electronegativity with Ca 2+ ions in the HdA structures. The easy-to-fabricate b-HdA can be employed as an effective industrial absorbent in the continuous-flow adsorption columns for the control of heavy metallic radionuclides from aqueous environments. Supplementary Materials: The following are available online at www.mdpi.com/xxx/s1, Table

Conclusions
In this work, spherical b-HdA with an approximate diameter of 2.0 mm was successfully prepared via a sintering process. The prepared b-HdA had a well-crystallized and mesoporous structure with a BET specific surface area of 34.91 m 2 /g and a maximum specific adsorption of 7.73 mg/g b-HdA for Co(II) at 293 K. The adsorption behaviors and mechanisms of Co(II) ions onto the b-HdA could be explained well using the Sips isotherm model and the pseudo-second-kinetic model, indicating the heterogeneous surface property of b-HdA. The adsorption capacity was increased with an increase in temperature, along with the thermodynamic parameters, indicating that the adsorption of Co(II) onto the b-HdA was thermodynamically favorable and spontaneous. Furthermore, intraparticle diffusion controlled the uptake of Co(II) onto the b-HdA as a rate-limiting step. The selective order of the b-HdA in a mixture of radionuclides was U(VI) > Co(II) > Ni(II) > Sr(II) > Cs(I) due to the impact of electronegativity with Ca 2+ ions in the HdA structures. The easy-to-fabricate b-HdA can be employed as an effective industrial absorbent in the continuous-flow adsorption columns for the control of heavy metallic radionuclides from aqueous environments.